A liquid crystal display apparatus includes semiconductor elements placed at intersection points between scanning wires and signal wires. Each semiconductor element includes: a semiconductor layer having a channel region and a pair of semiconductor regions which sandwich the channel region and which are each made of a high-resistance region and a low-resistance region; a first electrode formed on the intrinsic semiconductor region with an insulating film interposed therebetween; and second and third electrodes connected to the low-resistance regions. Each scanning wire constitutes the first electrode of the corresponding one of the semiconductor elements. The first electrode has a first wiring formed on the insulating film and second wiring formed in direct contact with a side surface of the first wiring, part of the second wiring being overlaid on part of a high-resistance region with the insulating film interposed therebetween.
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9. A liquid crystal display apparatus comprising:
a pair of substrates at least one of which is transparent; and a liquid crystal layer sandwiched between said pair of substrates; wherein one of said pair of substrates has a display region and a region of driving circuits for driving said display region; wherein said display region has a plurality of first semiconductor elements arranged in a matrix fashion; wherein the driving circuit region has a plurality of second semiconductor elements; wherein each of said pluralities of first and second semiconductor elements includes: a semiconductor layer having a channel region and a pair of semiconductor regions of a given conductivity type which sandwich said channel region and which are each made of a high-resistance region and a low-resistance region; and an electrode formed on said channel region with an insulating film interposed therebetween; and wherein said electrode has a first wiring formed on said insulating film and a second wiring formed on said first wiring such that said second wiring is directly in contact with a side surface of said first wiring, part of said second wiring being overlaid on part of the high-resistance regions of said pair of semiconductor regions of said given conductivity type with said insulating film interposed therebetween.
5. A liquid crystal display apparatus comprising:
a pair of substrates at least one of which is transparent; and a liquid crystal layer sandwiched between said pair of substrates; wherein one of said pair of substrates has a plurality of scanning wires, a plurality of signal wires intersecting said scanning wires in a matrix fashion, and a plurality of semiconductor elements placed at intersection points between said scanning wires and said signal wires; wherein said plurality of scanning wires have a first wiring layer and a second wiring layer formed in direct contact with a side surface of the first wiring layer; wherein each of said plurality of semiconductor elements includes: a semiconductor layer having a channel region and a pair of semiconductor regions of a given conductivity type which sandwich said channel region and which are each made of a high-resistance region and a low-resistance region; and an electrode formed on said channel region with an insulating film interposed therebetween; and wherein each of the electrodes in said plurality of semiconductor elements is comprised of the corresponding one of said plurality of scanning wires, part of said second wiring layer being overlaid on part of the high-resistance regions of said pair of semiconductor regions of said given conductivity type with said insulating film interposed therebetween.
1. A liquid crystal display apparatus comprising:
a pair of substrates at least one of which is transparent; and a liquid crystal layer sandwiched between said pair of substrates; wherein one of said pair of substrates has a plurality of scanning wires, a plurality of signal wires intersecting said scanning wires in a matrix fashion, and a plurality of semiconductor elements placed at intersection points between said scanning wires and said signal wires; wherein each of said plurality of semiconductor elements includes: a semiconductor layer having a channel region and a pair of semiconductor regions of a given conductivity type which sandwich said channel region and which are each made of a high-resistance region and a low-resistance region; a first electrode formed on said channel region with an insulating film interposed therebetween; and a second and a third electrode connected to the low-resistance regions of said pair of semiconductor regions of said given conductivity type; wherein each of said plurality of scanning wires comprises said first electrode of the corresponding one of said plurality of semiconductor elements; and wherein said first electrode has a first wiring formed on said insulating film and a second wiring formed on said first wiring such that said second wiring is directly in contact with a side surface of said first wiring, part of said second wiring being overlaid on part of the high-resistance regions of said pair of semiconductor regions of said given conductivity type with said insulating film interposed therebetween.
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The present invention relates to semiconductor elements and a liquid crystal display apparatus. More particularly, the invention relates to an active matrix liquid crystal display apparatus of high image quality incorporating highly reliable thin film semiconductor elements.
There exist active matrix liquid crystal display apparatuses incorporating thin film transistors (TFTs) to display image and text information in combination with OA equipment. For researchers working on this type of liquid crystal display, attaining higher resolution and higher image quality than ever has been a crucial task in addition to the efforts at lowering fabrication costs. To meet the challenges requires improving the performance of TFTs, i.e., a key device of the liquid crystal display. An attempt to form high-performance TFTs on an inexpensive glass substrate is disclosed illustratively in IEEE Transaction on Electron Devices, 1989, Vol. 36, pp. 351-359. The disclosure involves using TFTs to constitute peripheral drivers for driving a TFT active matrix, the TFTs being integrated on a single substrate to reduce fabrication costs. If advanced peripheral drivers are integrated on a glass substrate, the structure of circuits to be mounted externally and their assembling processes will be more simplified, which will translate into substantially reduced mounting costs. To devise a high-performance circuit configuration requires adopting more advanced TFTs than ever before. Today, TFTs formed on a polysilicon film (poly-Si TFTs) are hailed for effective use in liquid crystal display apparatuses that integrate peripheral drivers. In order to form a liquid crystal display apparatus with integrated peripheral drivers on an inexpensive glass substrate, it is necessary to reduce to 350°C C. or lower the temperature of a process in which to form the TFTs. In such a low-temperature process, the quality of gate insulating films of the TFTs is not as high as that of thermal oxidation films fabricated at a higher temperature. The comparatively low quality of the TFTs can trigger deterioration of the elements attributable to the injection of hot carriers. In recent years, the mobility of carriers within TFTs has been improved since the introduction of high-quality polysilicon film fabrication technology using laser recrystallization. This has also drawn attention to the importance of viable solutions to the problem of element deterioration. Obviously, degraded TFT characteristics can directly affect the quality of image display; images can flicker or lose their contrast factor due to the concomitant deterioration in the characteristics of drivers or pixel switching elements.
The phenomenon of element deterioration attributable to hot carriers is known to be triggered by high electric fields near drain junctions of transistors. As ways to prevent such degradation, a number of structures have been proposed to attenuate the drain junction field in submicron-order transistors used in silicon LSIs. Illustratively, a dual diffusion drain (DDD) structure having arsenic (As) and phosphorus (P) diffused therein is discussed in IEEE Transaction on Electron Devices, 1983, Vol. 30, pp. 652-657. A lightly doped drain (LDD) structure is proposed in IEEE Transaction on Electron Devices, 1980, Vol. 27, pp. 1359-1367. The proposed LDD structure involves having a low-density impurity diffusion layer interposed between a channel segment and a drain diffusion layer. This structure has since gained widespread acceptance in LSI devices. Some adverse phenomena specific to the LDD structure are minimized by the so-called gate overlapped drain (GOLD) structure having low-density impurity diffusion layers and part of gate electrodes overlapping one another with insulating films interposed therebetween, as proposed in IEEE Transaction on Electron Devices, 1988, Vol. 35, pp. 2088-2093.
Meanwhile, higher levels of resolution and larger display screens of liquid crystal display apparatuses have created a serious problem: signal delays caused by finite wiring resistance and wiring capacity. A number of wiring structures using low-resistance materials such as aluminum (Al) and copper (Cu) have been proposed as solutions to that problem. Illustratively, Japanese Patent Laid-open No. Sho 64-35421 discloses a wiring structure having a metal subject to high anodic oxidation and a metal of high electrical conductivity stacked one upon another.
The GOLD structure is highly effective in improving the reliability of transistors by substantially reducing peak values of drain junction fields therein. As such, the GOLD structure is thought to be an effective way to enhance the reliability of polysilicon TFTs used in liquid crystal display apparatuses. One disadvantage of the GOLD structure is that its complicated element constitution necessitates installation of elaborate fabrication processes. This has proved to be a severe problem for liquid crystal display apparatuses because cost reduction is one of their top priorities. It is difficult to implement the proposed structure unmodified as has been applied to silicon LSIs so far.
It is therefore an object of the present invention to overcome the above and other deficiencies of the prior art and to provide a highly reliable TFT structure that may be formed with a minimum of additional fabrication processes. Another object of the present invention is to provide, in addition to the dependable TFTs, a low-resistance wiring structure suitable for a liquid crystal display apparatus having a wide, fine-resolution screen.
In carrying out the invention and according to one aspect thereof, there is provided a liquid crystal display apparatus comprising a pair of substrates, one of which has a plurality of scanning wires, a plurality of signal wires intersecting the scanning wires in a matrix fashion, and a plurality of semiconductor elements placed at intersection points between the scanning wires and the signal wires. Each of the plurality of semiconductor elements includes: a semiconductor layer having an intrinsic semiconductor region and a pair of semiconductor regions of a given conductivity type which sandwich the intrinsic semiconductor region and which are each made of a high-resistance region and a low-resistance region; a first electrode formed on the intrinsic semiconductor region with an insulating film interposed therebetween; and a second and a third electrode connected to the low-resistance regions of the pair of semiconductor regions of the given conductivity type. Each of the plurality of scanning wires constitutes the first electrode of the corresponding one of the plurality of semiconductor elements. The first electrode has first wiring formed on the insulating film and second wiring formed on the first wiring, part of the second wiring being overlaid on part of the high-resistance regions of the pair of semiconductor regions of the given conductivity type with the insulating film interposed therebetween.
In a preferred structure according to the invention, the second wiring may be formed so as to cover the first wiring. The second wiring may preferably be formed on sides of the first wiring. Ends of the second wiring may be tapered.
In a further preferred structure according to the invention, the low-resistance regions of the pair of semiconductor elements of the given conductivity type may be formed in self-aligned relation to the second wiring. With this structure, boundaries of the low-resistance regions which are viewed in perpendicular relation to the substrates may coincide with boundaries of the second wiring which are viewed in perpendicular relation to the substrates.
In yet another preferred structure according to the invention, the second wiring may be formed on the first wiring with an insulating film interposed therebetween. With this structure, the first and the second wiring may be connected via contact holes to ensure the same potential over the wiring.
According to the invention, the first electrode (gate electrode) of each semiconductor element (TFT) and the high-resistance semiconductor layer are arranged to overlap to form the so-called GOLD structure. This structure allow the resistance of the high-resistance semiconductor layer to be controlled (i.e., lowered) by the gate electrode. That in turn attenuates electrical fields in the high-resistance semiconductor layer to forestall element deterioration caused by the injection of hot carriers into an insulating film over the high-resistance semiconductor layer, a phenomenon specific to the LDD structure. Lowering the resistance of the high-resistance semiconductor layer prevents lessening, due to the presence of that layer, of the ability of the elements to drive currents. Such improvements combine to provide highly reliable TFTs offering an enhanced current driving capability.
A minimum process increase is required to implement the above structure: a process for forming and patterning the second wiring need only be added.
It is not mandatory to cover the first wiring with the second wiring as long as the second wiring is kept equal in potential to the first wiring. That is, the second wiring may be formed on the first wiring with an insulating film interposed therebetween. In this case, however, the first and the second wiring must be connected outside the elements.
When the first wiring is isolated from the second wiring by the insulating film, the two kinds of wiring may be arranged to constitute an additional capacity to retain electrical charges. If the thickness of a second insulating film is suitably reduced, the added capacity increases the capacity value per unit area while the area occupied by that capacity is lessened. This contributes to enlarging the numerical aperture of pixels.
The GOLD structure above is effective not only in enhancing the reliability of TFTs but also in suppressing leak currents through TFTs attributable to photoelectric currents. With the active matrix liquid crystal display apparatus, lighting coming from backlight devices is switched on and off by liquid crystal. On that apparatus, the TFTs are necessarily exposed to the backlight. A light beam hitting any TFT causes the internal photoelectric effect within a semiconductor layer to generate electron-hole pairs flowing as a current. What is worrying in particular is an increase of leak currents when the TFTs are turned off. The problem becomes pronounced with projection type display apparatuses because of high levels of light intensity involved. Photoelectric leak currents are known to appear particularly in high electrical field regions close to drains. The problem may be bypassed when the low-resistance semiconductor layer is formed in self-aligned relation to the second wiring, i.e., when the entire top surface of the high-resistance semiconductor layer subject to high electrical fields is covered with the second wiring. This arrangement prevents light from reaching the regions most prone to generate photoelectric currents, thereby implementing TFTs with small leak currents.
Preferably, ends of the second electrodes may be tapered by etching. This structure helps prevent disconnected staggers in staggered portions of the top-layer wiring.
Generally, it is difficult during the taper etching process to control pattern dimensions within a large-area substrate. In a single-drain structure in which gate electrodes form only a single layer, variations in the pattern dimensions translate unmitigated into variations of TFT gate lengths. This results in irregularly distributed current driving capabilities of the TFTs over the substrate, making uniform image displays difficult.
Since the TFT gate length is defined by the fabricated size of the first wiring, the tapering of the second wiring by anisotropic etching of high pattern accuracy makes it possible both to ease the staggered configuration and to control the gate length with high precision. Although tapering the second wiring necessarily entails its dimensional variations which add to variations in the overlapping length of the gates and high-resistance semiconductor layer, such variations in the second wiring dimensions are not associated with the gate length. Because variations in the overlapping length do not affect the current driving capability of the TFTs as much as variations in the gate length, the uniformity of TFT characteristics within the substrate surface is not adversely affected by the tapered formation.
The first wiring may be formed preferably by any one of elements Si, Nb, Ta, Mo, W, Al, Ti, Fe, Cr, V and Zr; or by an ally of Si or N and any one of Nb, Ta, Mo, W, Al, Ti, Fe, Cr, V and Zr. The second wiring may be formed preferably by any one of Nb, Ta, Mo, W, Al, Ti, Fe, Cr, V and Zr; or by an ally of Si or N and any one of Nb, Ta, Mo, W, Al, Ti, Fe, Cr, V and Zr. The first and the second wiring may both be made of the same material.
Other objects, features and advantages of the present invention will become more apparent in the following specification and accompanying drawings.
The best mode for carrying the invention will now be described with reference to the accompanying drawings.
The pairs of high-resistance polysilicon layers 310 and 320 are in contact with a low-resistance n-type polysilicon layers 31 and a low-resistance p-type polysilicon layer 32 respectively. First gate wiring 10 made of aluminum is formed on these polysilicon layers, with an SiO2 gate insulating film 20 interposed therebetween. The first gate wiring 10 is covered with second gate electrodes 11 made of Nb. These components are all covered with an interlayer insulating film 22 made of SiO2. Through contact holes made in the interlayer insulating film 22, drain electrodes 12 and source electrodes 13 are connected to the low-resistance polysilicon layers 31 and 32. The entire element is covered with a protective insulating film 23 made of Si3N4.
As a characteristic of the first embodiment, the pair of high-resistance polysilicon layers 310 or 320 are formed in self-aligned relation to the pattern of the first gate wiring 10. In other words, the boundaries between the intrinsic polysilicon layer 30 and the high-resistance polysilicon layers 310 or 320 coincide with the pattern edges of the first gate electrodes 10. Part of the second gate electrodes 11 and part of the high-resistance polysilicon layers 310 or 320 are arranged to overlap, with the gate insulating film interposed therebetween.
When part of the gate electrodes and part of the high-resistance polysilicon layers 310 and 320 are overlaid to have the gate electrodes reduce the resistance of the polysilicon layers, the intensity of lateral fields in the high-resistance polysilicon layers 310 and 320 is eased and the reliability of the elements is thereby enhanced. Because the first embodiment utilizes low-resistance aluminum to make up the first gate electrodes 10, signal delays caused by the wiring resistance are lessened. That in turn contributes to making the display apparatus wider in area and finer in resolution than before.
Where aluminum components are covered with niobium (Nb), growth of aluminum hillocks is inhibited during heat treatment. This forestalls short-circuiting between the aluminum components and the wiring thereon.
The second embodiment uses Nb to constitute the first gate electrodes and NbN to make up the second gate electrodes. The second gate electrodes are formed only on sides of the first gate electrodes as follows: an NbN film is first formed all over the substrate, and then etched by a strongly anisotropic reactive ion etching method. In functional terms, the second gate electrodes 11 are connected to the first gate electrodes 10 as in the case of the first embodiment. This also eases the intensity of lateral fields in the high-resistance polysilicon layers 310 and 320 and thereby improves the reliability of the elements. Because the second embodiment has no need for a photo resist forming process to fabricate the second gate electrodes 12, the production steps are made simpler and the cost of manufacture is lowered.
Because the gate length of the TFTs is determined by the fabricated dimensions of the first gate wiring, the first gate wiring is formed perpendicularly by anisotropic etching of high pattern precision, with the second gate wiring tapered on top. This structure helps ease the staggered configuration and control the gate length accurately at the same time. The second gate wiring when tapered necessarily involves dimensional variations which add to variations in the overlapping length of the gates and high-resistance semiconductor layer. However, such variations in the second gate wiring dimensions are not associated with the gate length. Because variations in the overlapping length do not affect the current driving capability of the TFTs as much as variations in the gate length, the uniformity of TFT characteristics within the substrate surface is not adversely affected by the tapered formation. Thus the structure of the third embodiment not only prevents severed wires in the upper-layer wiring but also ensures uniform TFT characteristics inside the substrate.
The fifth embodiment is basically the same in structure as the first embodiment except that the first gate electrodes 10 are isolated from the second gate electrodes 11 by an insulating film 24. As depicted in
The vertical scanning circuit 51 and horizontal scanning circuit 53 are each constituted by shift registers and buffers shown in FIG. 11 and are driven by clock signals CL1, C12 and CKV. In
Incorporating the inventive TFTs into the active matrix display and driving circuit makes it possible to constitute a highly reliable display apparatus free of image quality degradation.
In the TFTs of this embodiment, the first and second gate electrodes 10 and 11 are isolated from one another by the insulating film 24. The first and second gate electrodes 10 and 11 are interconnected by the connection electrodes 17 that pass through holes in the second gate electrodes 11 and insulating film 24 as well as through contact holes TH1 in the interlayer insulating film 22.
As depicted in
As described, placing the insulating layer 24 between two layers of gate electrodes for isolation purposes allows the components involved to constitute an additional capacity. The capacity thus added may be increased per unit area by suitably reducing the thickness of the insulating film 24. When the area occupied by the added capacity is reduced, the pixel numerical aperture is improved. With the deterioration of the TFTs forestalled as in other embodiments of this invention, the TFTs above obviously make up another factor contributing to the implementation of a fine-resolution display apparatus.
This liquid crystal display apparatus is assembled by first forming separately the layers on the glass substrate 1 and on the opposite glass substrate 508. The upper and lower glass substrates 1 and 508 are then positioned face to face and arranged to contain the liquid crystal 506 therebetween. Transmitted light from backlights BL is adjusted by the pixel electrodes 14, which constitutes a TFT-driven color liquid crystal display apparatus. When the semiconductor elements discussed above are used as TFTs for driving the pixel electrodes 14 and as TFTs of the driving circuit, a highly reliable fine-resolution TFT type liquid crystal display apparatus is implemented.
Steps to fabricate the TFTs shown in
An SiO2 film 21 serving as a buffer layer is deposited to a thickness of 300 nm by plasma CVD on the glass substrate 1. Amorphous silicon (a-Si) film is then deposited to 35 nm thick by plasma CVD. The amorphous silicon film is patterned as desired by a known photolithography method. The patterned silicon film is subjected to irradiation of XeCl excimer laser (with wavelength of 308 nm) for recrystallization, which provides a polysilicon (poly-Si) film 30 (FIG. 18).
An SiO2 film 20 serving as a gate insulating film is deposited to a thickness of 80 nm by plasma CVD. Aluminum (Al) is then deposited by sputtering to 150 nm thick and patterned into first gate electrodes 10. With the p-type TFTs protected by a photo resist, phosphorus (P) is injected only into the n-type TFTs at 1×1014 (cm-2) using the first gate electrodes 10 as a mask. This forms a high-resistance n-type polysilicon layer 310. The same step is repeated on the p-type TFTs to form a high-resistance p-type polysilicon film 320. In the latter process, boron (B) is injected instead of phosphorus (FIG. 19).
An Nb film is deposited to a thickness of 200 nm by sputtering. The deposited film is patterned so as to cover the first gate electrodes 10, whereby second gate electrodes 11 are obtained. With the p-type TFTs protected by a photo resist, phosphorus (P) is injected only into the n-type TFTs at 3×1015 (cm-2) using the first gate electrodes 10 as a mask. This forms a low-resistance n-type polysilicon layer 31. The same step is repeated on the p-type TFTs to form a low-resistance p-type polysilicon layer 32. In the latter process, boron (B) is injected instead of phosphorus.
XeCl excimer laser (with wavelength of 308 nm) is again applied. The laser irradiation activates the injected impurities (FIG. 20).
An SiO2 film serving as an interlayer insulating film 22 is deposited to a thickness of 400 nm by plasma CVD, and contact holes are made therein. A CrMo alloy film is then deposited to 400 nm thick by sputtering and patterned into source and drain electrodes. An Si3N4 film acting as a protective insulating film 23 is deposited to 500 nm thick by plasma CVD, and contact holes are made therein. Lastly, an ITO film is deposited to 70 nm thick by sputtering and patterned into pixel electrodes 14 (FIG. 21).
The above embodiment of the invention permits fabrication of a highly reliable TFT active matrix with low-resistance gate wiring by simply adding the process of forming the second gate electrodes. Any increase in the cost of manufacturing is thus minimized.
Steps to fabricate the TFTs shown in
An SiO2 film 21 serving as a buffer layer is deposited to a thickness of 300 nm by plasma CVD on the glass substrate 1. Amorphous silicon (a-Si) film is then deposited to 35 nm thick by plasma CVD. The amorphous silicon film is patterned as desired by a known photolithography method. The patterned silicon film is subjected to irradiation of XeCl excimer laser (with wavelength of 308 nm) for recrystallization, which provides a polysilicon (poly-Si) film 30. The steps up to this point are the same as those applicable to FIG. 18 and will not be illustrated further.
An SiO2 film 20 serving as a gate insulating film is deposited to a thickness of 80 nm by plasma CVD. The deposited film is patterned into first gate electrodes 10. With the p-type TFTs protected by a photo resist, phosphorus (P) is injected only into the n-type TFTs at 1×1014 (cm2) using the first gate electrodes 10 as a mask. This forms a high-resistance n-type polysilicon layer 310. The same step is repeated on the p-type TFTs to form a high-resistance p-type polysilicon film 320. In the latter process, boron (B) is injected instead of phosphorus (FIG. 22).
An NbN film is deposited to a thickness of 400 nm by sputtering. The deposited film is subjected to anisotropic etching using reactive ions. The process fabricates second gate electrodes 11 in the form of side walls on sides of the first gate electrodes 10. With the p-type TFTs protected by a photo resist, phosphorus (P) is injected only into the n-type TFTs at 3×1015 (cm-2) using the first gate electrodes 10 as a mask. This forms a low-resistance n-type polysilicon layer 31. The same step is repeated on the p-type TFTs to form a low-resistance p-type polysilicon layer 32. In the latter process, boron (B) is injected instead of phosphorus. XeCl excimer laser (with wavelength of 308 nm) is again applied to activate the injected impurities (FIG. 23).
An SiO2 film serving as an interlayer insulating film 22 is deposited to a thickness of 400 nm by plasma CVD, and contact holes are made therein. A CrMo alloy film is then deposited to 400 nm thick by sputtering and patterned into source and drain electrodes. An Si3N4 film acting as a protective insulating film 23 is deposited to 500 nm thick by plasma CVD, and contact holes are made therein. Lastly, an ITO film is deposited to 70 nm thick by sputtering and patterned into pixel electrodes 14 (FIG. 24).
The above embodiment of the invention eliminates the need for a photolithography process in forming the second gate electrodes. This makes it possible to fabricate a highly reliable TFT active matrix at reduced costs.
Steps to fabricate the TFTs shown in
An SiO2 film 21 serving as a buffer layer is deposited to a thickness of 300 nm by plasma CVD on the glass substrate 1. Amorphous silicon (a-Si) film is then deposited to 35 nm thick by plasma CVD. The amorphous silicon film is patterned as desired by a known photolithography method. The patterned silicon film is subjected to irradiation of XeCl excimer laser (with wavelength of 308 nm) for recrystallization, which provides a polysilicon (poly-Si) film 30 (FIG. 25).
An SiO2 film 20 serving as a gate insulating film is deposited to a thickness of 80 nm by plasma CVD. An Nb film is then deposited by sputtering to 150 nm thick and patterned into first gate electrodes 10. The gate insulating film 20 is patterned successively using the first gate electrodes 10 as a mask. With the p-type TFTs protected by a photo resist, phosphorus (P) is injected only into the n-type TFTs at 1×1014 (cm-2) using the first gate electrodes 10 as a mask. This forms a high-resistance n-type polysilicon layer 310. The same step is repeated on the p-type TFTs to form a high-resistance p-type polysilicon film 320. In the latter process, boron (B) is injected instead of phosphorus (FIG. 26).
An SiO2 film 24 is then deposited to 100 nm thick by plasma CVD, followed by an Nb film deposited to a thickness of 100 nm by sputtering and patterned so as to cover the first gate electrodes 10. This process fabricates second gate electrodes 11. With the p-type TFTs protected by a photo resist, phosphorus (P) is injected only into the n-type TFTs at 3×101 (cm-2) using the first gate electrodes 10 as a mask. This forms a low-resistance n-type polysilicon layer 31. The same step is repeated on the p-type TFTs to form a low-resistance p-type polysilicon layer 32. In the latter process, boron (B) is injected instead of phosphorus. XeCl excimer laser (with wavelength of 308 nm) is again applied to activate the injected impurities (FIG. 27).
An SiO2 film serving as an interlayer insulating film 22 is deposited to a thickness of 400 nm by plasma CVD, and contact holes are made therein. A CrMo alloy film is then deposited to 400 nm thick by sputtering and patterned into source and drain electrodes. An Si3N4 film acting as a protective insulating film 23 is deposited to 500 nm thick by plasma CVD, and contact holes are made therein. Lastly, an ITO film is deposited to 70 nm thick by sputtering and patterned into pixel electrodes 14 (FIG. 28).
The above embodiment causes impurities to be injected directly into the polysilicon film, i.e., without penetration through an insulating film. This means that ion injection can take place at a significantly lowered level of energy. Specifically, an acceleration voltage of 5 kV or less permits injection of ions. The low-voltage impurity injection reduces damage to the protective resist during the ion injection process, allowing the resist to be peeled off more easily at the end of the process. Because an unsophisticated device is sufficient for carrying out the low-voltage ion injection, the outlay for equipment is reduced and so are the manufacturing costs.
As described and according to the invention, highly reliable semiconductor elements (TFTs) are formed with a minimum of increase in the fabrication steps. This makes it possible to manufacture at low costs a liquid crystal display apparatus affording fine resolution with little image quality degradation.
The invention is thus carried out to implement a low-resistance wiring structure that helps build a wide-screen high-resolution liquid crystal display apparatus with little deterioration in its image quality.
As described, the inventive liquid crystal display apparatus is constituted by highly reliable semiconductor elements fabricated with a minimum of increase in fabrication processes. At the same time, the apparatus embraces a low-resistance wiring structure conducive to producing a large-screen fine-resolution display with little image degradation.
Kageyama, Hiroshi, Kawachi, Genshiro, Mikami, Yoshiro, Masuda, Kazuhito, Ohkubo, Tatsuya
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